The flexibility of A-form DNA.

We have determined the rise per base pair and persistence length of A-form DNA in trifluoroethanol solutions for fragments 350-900 base pairs in length that best describe rotational diffusion coefficients determined by transient electric birefringence. The 2.6 A spacing between base pairs found in crystal and fiber A-form structures is preserved in solution. The persistence length is about 1500 A, or about three times longer than for B-form DNA. There is no apparent electrostatic contribution to the persistence length in the salt concentration range 0.2-2.0 mM Na cacodylate. This suggests an even closer association between DNA and its neutralizing counterions than predicted by condensation theory, perhaps due to a sheath of trifluoroethanol excluded water surrounding the A-form helix.     

The Flexibility of Alternating dA—dT Sequences

Abstract

The flexibility of alternating poly (dA—dT) has been investigated by the technique of transient electric dichroism. Rotational relaxation times, which are very sensitive to changes in the end-to-end length of flexible polymers, are determined from the field free dichroism decay curves of four, well defined fragments of poly (dA—dT) ranging in size from 136 to 270 base pairs. Persistence lengths, calculated from the results of Hagerman and Zimm (Biopolymers (1981) 29, 1481–1502), are in the range 200–250 A. This makes alternating dA—dT sequences about twice as flexible as naturally occurring, “random” sequence DNA. Considering a bend around a nucleosome, for example, this difference in persistence length translates to an energy difference between poly (dA—dT) and random sequence DNA of 0. 17 kT/base pair or 1 kcal per 10 base pair stretch. This energy difference is sufficiently large to suggest that dA—dT sequences could serve as markers in DNA packaging, for example, at sites where DNA must tightly bend to accommodate structures.     

Peculiarities of the B to A Transition of the λ Phage Regulatory Site OR3 and of Its Fragment

Abstract

Conformations of the synthetic deoxyoligonucleotide 17 base pairs long, which is an OR3 operator of λ phage, and of its 9-b.p. fragment were studied by the circular dichroism method (CD). The regions of stability of the double-stranded state were determined for these duplexes. A comparison of the CD spectra for these oligonucleotides with the CD for a lengthy DNA showed the conformation of these short DNA pieces to belong to the B-family.

A cooperative change in the CD spectra is observed in trifluoroethanol (TFE) solutions at a TFE concentration specific for each oligonucleotide, which is supposed to stem from a B to A transition. The length of the fragment was found to affect the ability for the B-A transition. The transition into the A form is hindered by 13% TFE for the short 9-nucleotide in comparison with the 17-nucleotide. We suggest that this is due to the B form stabilization by terminal base pairs (B-phility of the ends).     

Conformation and circular dichroism of DNA.

CD spectra of calf thymus, C. perfringens, E. coli, and M. luteus DNA have been measured in the vacuum-uv region to about 168 nm for the A-, B-, and C-forms. The positive band at about 187 nm and the negative band at about 170 nm found for each type and form of DNA are sensitive to the source of the DNA and the base–base interactions of the double-stranded helix. The A-form spectra confirm that these bands are indeed sensitive to secondary structure. In the near-uv, the CD of B-form DNA is well analyzed as a linear combination of 27% A-form and 78% C-form. However, an analysis of the extended spectrum demonstrates that the near-uv analysis is not correct. The extended analysis shows that the base–base interactions are similar for B- and C-forms in solution, which implies that these two forms have nearly the same number of base pairs per turn. Various types of CD difference spectra are also discussed.     

Comparative Studies of the Thermodynamic Stabilities Between Sheared A:G and Watson-Crick A:U(T) Base Pairs in RNA and DNA

Abstract

Thermodynamic parameters for duplex formation were determined from CD melting curves for r(GGACGAGUCC)₂ and d(GGACGAGTCC)₂, both of which form two consecutive ‘sheared’ A:G base pairs at the center [Katahira et al. (1993) Nucleic Acids Res. 21, 5418–5424; Katahira et al., (1994) Nucleic Acids Res. 22, 2752–27591. The parameters were determined also for r(GGACUAGUCC)₂ and d(GGACTAGTCC)₂, where the A:G mismatches are replaced by Watson-Crick A:U(T) base pairs. Thermodynamic properties for duplex formation are compared between the sheared and the Watson-Crick base pairs, and between RNA and DNA. Difference in the thermodynamic stability is analyzed and discussed in terms of enthalpy and entropy changes. The characteristic features in CD spectra of RNA and DNA containing the sheared A:G base pairs are also reported.

     

Structural Property of DNA That Migrates Faster in Gel Electrophoresis,as Deduced by CD Spectroscopy

Bent DNAs are known to migrate slower than ordinary DNA in non-denaturing polyacrylamide gel electrophoresis. In contrast, several satellite DNAs have been shown to migrate fast. The structural property that causes the fast migration, however, is not clarified so far on molecular basis. We have investigated the structural property of a satellite DNA, which contains consecutive purine sequences and migrates faster in gel, by CD spectroscopy. Partial formation of an A-form–like structure has been suggested. Reduction in DNA length due to the formation of the A-form–like structure may be responsible for the fast migration. The pronounced rigidity of DNA may also contribute to the behavior.     

Structures of Non-canonical Tandem Base Pairs in RNA Helices: Review

Abstract

The structures of tandem non-canonical base pairs, a frequently recurring motif in RNA molecules, are reviewed and analysed. The tandem non-canonical base pair motifs can be roughly divided in three groups, containing seven subgroups based on their base pairing patterns and local geometries. Structural details and helical parameters that can be used to numerically distinguish between the subgroups are tabulated. Remarkably, while the individual helical twists of the tandem and adjacent base pair steps can be substantially smaller or larger than the typical A-form value of 32.7°, the average value is close to A-form. This and other striking regularities resulting from compensating geometrical adjustments, important for understanding and predicting the configurations of non-canonical base pairs geometries are discussed.     

Alternation of DNA and Solvent Layers in the A Form of d(GGCGCC) Obtainhted by Ethanol Crystallization

Abstract

We have determined by X-ray crystallography the structure of the hexamer duplex d(GGCGCC)₂ in the A-form using ethanol as a precipitant. The same sequence had previously been crystallized in the B-form, but with 2-methyl-2, 4-pentanediol as a precipitant. It appears that ethanol precipitation is a useful method to induce the formation of A-form crystals of DNA. Packing of the molecules in the crystal has unique features: the known interaction of A-DNA duplexes between terminal base-pairs and the minor groove of neighbor molecules is combined with a superstructure consisting in an alternation of DNA layers and solvent layers (water/ions). This organization in layers has been observed before, also with hexamers in the A conformation which crystallize in the same space group (C222 ₁). The solvent layer has a precise thickness, although very few ordered water molecules can be detected. Another feature of this crystal is its large unit cell, which gives rise to an asymmetric unit with three hexamer duplexes. One of the three duplexes is quite different from the other two in several aspects: the number of base pairs per turn, the twist pattern, the mean value of the twist angle and the fact that one terminal base-pair is not stacked as part of the duplex and appears to be disordered. So the variability in conformation of this sequence is remarkable.     

Abolition of Intrinsically Bent DNA Structure Components in AT Clusters by Netropsin Interaction; Titration Viscometric Investigations

Abstract

It is argued that the enhancement of the apparent DNA contour length by the specifically binding non-intercalating drug netropsin (Nt) (Reinert et al., NAR 9,2335, 1981) at very low Nt/DNA-phosphate ratios essentially is the result of an abolition of periodically arranged intrinsic helix bends in A · T rich tracts of base pairs.

In the preceding paper the existence of pronounced DNA tertiary structure components has been postulated for (two species of) natural eukaryotic DNA. The resulting model suggests local apparent solenoid-related DNA tertiary structure components at high sodium ion concentration c_s, partly/totally molten out at 45/60 C. With decreasing c_s the tertiary structure components have been found to be gradually reduced, at least below c_s = 0.010 M, as titration viscometrically revealed by a gradual rise of the apparent DNA contour length (Reinert et al., JBSD 9, 537, 1991).

Hence, we performed titration viscometric analyses about Nt interaction with calf thymus DNA (ctDNA) at c_s = 0.075 M, 0.010 M and 0.004 M Na⁺. The concomitant DNA conformational changes are quantitatively described in terms of the relative changes of both DNA persistence length and hydrodynamically operative apparent DNA contour length for the three first resolved interaction modes below a Nt/DNA-P ratio of 0.03.

These experiments, together with previous respective analyses at c_s = 0.20 M Na⁺ and different temperatures (I.e.), suggest that those DNA sites binding Nt most strongly predominantly are responsible for the formation of solenoid-related DNA tertiary structure components. Most probably these are A tract-containing sequences. As the essential factor for their apparent elongation effect at low Na⁺ concentrations, a gradual alteration of the number of base pairs per helix turn seems to occur below c_s = 0.010 M Na⁺ and, concomitantly, a change in phasing between intrinsic helix bends and helix screw.     

DNA orientation in shear flow

The linear dichroism (LD) has been measured for DNA molecules 239–164,000 base pairs long oriented in shear flow over a large range of velocity gradients (30–3,000 s ^?1) and ionic strengths (2–250 mM). At very low gradients, the degree of DNA orientation increases quadratically with the applied shear as predicted by the Zimm theory [J. Zimm, (1956) Chemical Physics, Vol. 24, p. 269]. At higher gradients, the orientation of fragments ≥ 7 kilobase pairs (kbp) increases linearly with increasing shear, whereas the orientation of fragments ≥ 15 kbp shows a more complicated dependence. In general, the orientation decreases with increasing ionic strength throughout the studied ionic strength interval, owing to a decrease in the persistence length of the DNA. The effect is most dramatic at ionic strengths below 10 mM, and is more pronounced for longer DNA fragments. For fragments ≥ 15 kbp and velocity gradients ≥ 100 s^?1, the orientation can be adequately described by the empirical relation: LD^r= –(k₁-G)/(k₂ + G), where k₁is a linear function of the square root of the ionic strength and k₂ depends on the DNA contour length. Since the DNA persistence length can be represented as a linear function of the reciprocal square root of the ionic strength [D. Porschke, (1991) Biophysical Chemistry, Vol. 40, p. 169], extrapolation of the empirical relation provides information about the stiffness of the DNA fibers. © 1993 John Wiley & Sons, Inc.     

Sequence and conformational effects on imino proton exchange in A.T- and A.U-containing DNA and RNA duplexes

¹H-nmr relaxation has been used to study the effect of sequence and conformation on imino proton exchange in adenine–thymine (A · T) and adenine–uracil (A · U) containing DNA and RNA duplexes. At low temperature, relaxation is caused by dipolar interactions between the imino and the adenine amino and AH2 protons, and at higher temperature, by exchange with the solvent protons. Although room temperature exchange rates vary between 3 and 12s^?1, the exchange activation energies (E_α) are insensitive to changes in the duplex sequence (alternating vs homopolymer duplexes), the conformation (B-form DNA vs A-form RNA), and the identity of the pyrimidine base (thymine vs uracil). The average value of the activation energy for the five duplexes studied, poly[d(A-T)], poly[d(A) · d(T)], poly[d(A-U)], Poly[d(A) · d(U)], and poly[r(A) · r(U)], was 16.8 ± 1.3 kcal/mol. In addition, we find that the average E_α for the A.T base pairs in a 43-base-pair restriction fragment is 16.4 ± 1.0 kcal/mol. This result is to be contrasted with the observation that the E_α of cytosine-containing duplexes depends on the sequence, conformation, and substituent groups on the purine and pyrimidine bases. Taken together, the data indicate that there is a common low-energy pathway for the escape of the thymine (uracil) imino protons from the double helix. The absolute values of the exchange rates in the simple sequence polymers are typically 3–10 times faster than in DNAs containing both A · T and G · C base pairs.     

Breathing and bending fluctuations in DNA modeled by an open-base-pair kink coupled to axial compression

We develop a model designed to show that flexibility in the DNA molecule can arise from relatively improbable transient opening of base pairs. The axial direction changes at the site of an open base pair. The region between open base pairs is a double helix of hydrogen-bonded base pairs with a slightly decreased rise per residue and a slightly increased helical winding angle. An analysis of the model yields several testable predictions. For example, we predict probability 0.026 for a base pair to be open at 25°C, a value close to that measured by hydrogen-exchange experiments. Other predictions involve matters like the variation of persistence length with ionic strength and temperature, the variation of helical winding angle with temperature, and the kinetics of heat denaturation. An additional result of the analysis is an explanation of the high degree of local stiffness of the DNA molecule. Strong resistance to bending fluctuations is provided from two sources: increased polyelectrolyte repulsion among phosphate groups in the axially compressed stacks between open base pairs and the tendency of stacking forces to oppose opening of a base pair. Stacking forces, however, also support compression of the stacks between open base pairs, so that the net effect of stacking forces on elastic bending of DNA is small relative to the polyelectrolyte effect. If the ionic charges on the phosphate groups were absent, DNA would spontaneously fold, driven by the entropy gained when about 1% of its base pairs open.     

Left-handed Z Form in Superhelical DNA: A Theoretical Study

Abstract

This is a comprehensive statistical mechanical treatment of the Z form formation in purine- pyrimidine stretches of different length inserted into superhelical DNA. The B-Z transition for short inserts is shown to follow the “all-or-none” principle. Over some critical value of the insert length n, the B-Z transition in the insert proceeds in two stages. The flipping of m base pairs into the Z form is followed by a gradual growth of the Z-form stretch until it occupies the whole insert. By fitting the theoretical transition curves to experimental ones the fundamental thermodynamic parameters of the B-Z transition have been determined: the B-Z junction energy Fj = 4–5kcal?mol^?1 and the free energy change ΔF_B-Z = 0.5–0.7 kcal?mol^?1 under standard salt conditions. Calculations show that the B-Z transition in short purine-pyrimidine inserts may be seriously affected by cruciform formation in the carrier DNA.     

Sedimentation of homogeneous double-strand DNA molecules.

Sedimentation velocity studies have been carried out with isolated double-strand DNA fragments prepared by digestion of PM2 phage with the restriction endonuclease Hae III. The results show that DNA molecules shorter than about 200 base pairs behave almost exactly as rigid rods with a diameter of 27 A. The behavior of the larger fragments (up to 1735 base pairs) can be described very well by either the theory of Yamakawa and Fujii (Yamakawa, H., and Fujii, M. (1973), Macromolecules 6. 407) using the same diameter and a persistence length of 575 A, or the theory of Hearst and Stockmayer (Hearst, J.E., and Stockmayer, W.H. (1962), J. Chem. Phys. 37, 1425) using a diameter of 20 A and a persistence length of 525 A.     

Studies on the Effect of Thymine-Mercury-Thymine Stem as a Structural or Functional Motif in DNAzymes

T-Hg-T base pair formation has been demonstrated to be compatible with duplex DNA context, with considerable thermal stability contribution. Here, the T-Hg-T stem in two small DNAzymes 8–17 and 10–23 was studied for its structural and functional roles. The recognition arm 5′ to the cleavage site of 10–23 DNAzyme complex and the stem in the catalytic loop of 8–17 DNAzyme could be replaced by consecutive T-Hg-T stem of different length. The linear relationship between the activity of the complex 10–23DZ-6T+D19–6T and the concentration of Hg²⁺ demonstrated that the T-Hg-T stem contributes thermal stability of the recognition arm binding. The effect of T-Hg-T stem in the catalytic core of 8–17 DNAzyme and the position-dependent effect in 10–23 DNAzyme demonstrated that T-Hg-T base pair is not compatible with canonical base pairs in playing the functions of nucleic acids.     

Helix-coil transition in nucleoprotein: renaturation of polylysine-DNA and polylysine-nucleohistone complexes

Thermal denaturation and renaturation of directly mixed and reconstituted polylysine–DNA, directly mixed polylysine–nucleohistone complexes, and NaCl-treated nucleohistones in 2.5 × 10^?4 M EDTA, pH 8.0 have been studied. At the same input ratio of polylysine to DNA, the percent of renaturation of free base pairs in a directly mixed polylysine–DNA complex is higher than that in a reconstituted complex. For a directly mixed complex, the renaturation of free base pairs is proportional to the fraction of DNA bound by polylysine or inversely proportional to the sizes of free DNA loops. A of large amount of renaturation of free base pairs has also been observed for 0.6 M and 1.6 M NaCl-treated nucleohistones. The binding of polylysine to nucleohistone enhances the renaturation of histone-bound base pairs. The percent of renaturation of polylysine–bound base pairs is high and is approximately independent of the extent of binding on DNA by polylysine. This is true in polylysine–DNA complexes prepared either by reconstitution or by directly mixing. It also applies for polylysine–nucleohistone complexes. The model where polylysine-bound base pairs collapse at T_m′ with two complementary strands still bound by polylysine is favored over the model where polylysine is dissociated from DNA during melting. The low renaturation of histone-bound base pairs in nucleo-histone indicates that either histones do not hold two complementary strands of DNA tightly or that histones are fully or partially dissociated from DNA when the nucleo-histone is fully denatured.     

A Raman Study of the Time Variability for the A-to-B Transition in Wet-spun Films of Calf-thymus DNA

Synopsis

The time evolution of the A-to-B transition has been monitored by Raman spectroscopy and found to vary significantly for different samples. Though all samples were prepared in the identical fashion, some samples completed the transition on the time scale of several hours while other samples took days. The shortest time required for the A conformation to disappear was about 2 hours, as determined by the disappearance of the A-form Raman band at 807 cm^?1. For these fastest transforming samples, the B-form Raman band at 835 cm^?1 was clearly evident after about 5 hours. These data are consistent with the hypothesis that the A conformation of DNA is stabilized by intermolecular interactions.     

The subunit structure of chromatin from Physarum polycephalum.

Nucleosome DNA repeat lengths in Physarum chromatin, determined by nuclease digestion experiments, are shorter than those observed in most mammalian chromatin and longer than those reported for chromatin of certain other lower eukaryotes. After digestion with staphylococcal nuclease for short periods of time an average repeat length of 190 base pairs is measured. After more extensive digestion an average repeat length of 172 base pairs is measured. Upon prolonged digestion DNA is degraded to an average monomer subunit length of 160 base pairs, with only a small amount of DNA found in lengths of 130 base pairs or smaller. Mathematical analysis of the data suggests that the Physarum nucleosome DNA repeat comprises a protected DNA segment of about 159 base pairs with a nuclease-accessible interconnecting segment which ranges from 13 to 31 base pairs. The spacing data are compatible with measurements from electron micrographs of Physarum chromatin.     

Sequence dependence of the B-A conformational transition of DNA

We have studied, by conformational analysis, the sequence dependence of DNA conformational transition between B- and A-forms. We have considered intramolecular interactions between base pairs, without backbone, to examine their role in the conformational transition between B- and A-forms, and found that base pairs themselves usually have intrinsic conformational preferences for the B- or A-form. Calculation of all ten possible base steps shows that the base combinations, CC (or GG), GC, AT, and TA, have tendencies to assume the A-conformation. Results show that it is particularly easy to slide along the long axis of the base pair for these steps, with AT and CC showing especially flat energies. These calculations show that a preference for the B- or A-conformation depends on the electrostatic energy parameters, in particular, on dielectric and shielding constants; the A-conformation is preferred for low dielectric constant or low shielding. Both the A- and B-conformations are mainly stabilized by electrostatic interactions between favorably juxtaposed atomic charges on base pairs; however, the B-conformation generally has more favorable van der Waals interactions than the A-form. These sequence-dependent conformational preference and environmental effects agree roughly with experimental observations, suggesting that the origin of the conformational polymorphism is attributable to the intrinsic conformational preference of base pairs.     

The flexibility of alternating dA-dT sequences

The flexibility of alternating poly (dA-dT) has been investigated by the technique of transient electric dichroism. Rotational relaxation times, which are very sensitive to changes in the end-to-end length of flexible polymers, are determined from the field free dichroism decay curves of four, well defined fragments of poly (dA-dT) ranging in size from 136 to 270 base pairs. Persistence lengths, calculated from the results of Hagerman and Zimm (Biopolymers (1981) 29, 1481-1502), are in the range 200-250 A. This makes alternating dA-dT sequences about twice as flexible as naturally occurring, "random" sequence DNA. Considering a bend around a nucleosome, for example, this difference in persistence length translates to an energy difference between poly (dA-dT) and random sequence DNA of 0.17 kT/base pair or 1 kcal per 10 base pair stretch. This energy difference is sufficiently large to suggest that dA-dT sequences could serve as markers in DNA packaging, for example, at sites where DNA must tightly bend to accommodate structures.